We build the distribution function for a system with coexisting self-locali
zed and delocalized fermions. The distribution function is used to study th
e behavior of the chemical potential of the carriers in such a system, whic
h is found to differ substantially from the behavior of the chemical potent
ial in a system of delocalized fermions. We also find that as the temperatu
re changes, isostructural first-order phase transitions can emerge in the s
ystem of self-localized and delocalized fermions. These transitions, for wh
ich changes in the state of the macroscopic number of particles are respons
ible, manifest themselves in the electrical conductivity, in the contributi
on of carriers to the specific heat, and in the optical properties of such
systems. Formulas are derived that approximate the dependence of the temper
ature of such a phase transition on the binding energy of the self-localize
d states of carriers and on the maximum group velocity of phonons participa
ting in the formation of such states. Finally, we show that the special fea
tures of the behavior of the chemical potential of the carriers in a system
with carrier self-localization lead to the possibility of Bose condensatio
n in a system where bipolaron states are metastable. (C) 1999 American Inst
itute of Physics. [S1063-7761(99)01910-1].